Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803025571/ob6317sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536803025571/ob6317Isup2.hkl |
CCDC reference: 227889
Data collection: SMART (Bruker, 2000); cell refinement: SMART; data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXTL (Bruker, 2000); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
C14H10BrN | F(000) = 2176 |
Mr = 272.14 | Dx = 1.538 Mg m−3 |
Orthorhombic, Fdd2 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: F 2 -2d | Cell parameters from 1496 reflections |
a = 47.219 (12) Å | θ = 2.4–20.6° |
b = 24.229 (6) Å | µ = 3.47 mm−1 |
c = 4.1085 (10) Å | T = 293 K |
V = 4700 (2) Å3 | Prism, colourless |
Z = 16 | 0.3 × 0.2 × 0.2 mm |
Bruker SMART CCD area-detector diffractometer | 2284 independent reflections |
Radiation source: fine-focus sealed tube | 1610 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.075 |
φ and ω scans | θmax = 26.0°, θmin = 1.9° |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | h = −58→52 |
Tmin = 0.43, Tmax = 0.50 | k = −29→24 |
6379 measured reflections | l = −5→4 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.045 | H-atom parameters constrained |
wR(F2) = 0.088 | w = 1/[σ2(Fo2) + (0.02P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.05 | (Δ/σ)max < 0.001 |
2284 reflections | Δρmax = 0.44 e Å−3 |
145 parameters | Δρmin = −0.34 e Å−3 |
1 restraint | Absolute structure: Flack (1983), 965 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.014 (15) |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane) 21.9209 (0.0998) x - 0.1847 (0.0528) y - 3.6388 (0.0046) z = 5.4707 (0.0434) * 0.0016 (0.0037) C2 * -0.0013 (0.0040) C3 * 0.0003 (0.0040) C4 * 0.0003 (0.0036) C5 * -0.0001 (0.0040) C6 * -0.0009 (0.0040) C7 Rms deviation of fitted atoms = 0.0009 16.4269 (0.1123) x + 2.4815 (0.0646) y + 3.8288 (0.0040) z = 7.6557 (0.0414) Angle to previous plane (with approximate e.s.d.) = 48.34 (0.14) * 0.0051 (0.0039) C8 * 0.0028 (0.0049) C9 * -0.0088 (0.0057) C10 * 0.0066 (0.0054) C11 * 0.0015 (0.0046) C12 * -0.0072 (0.0040) C13 Rms deviation of fitted atoms = 0.0059 |
x | y | z | Uiso*/Ueq | ||
Br | 0.272011 (12) | 0.65748 (2) | 0.49307 (17) | 0.0614 (2) | |
C1 | 0.30571 (10) | 0.62629 (18) | 0.2846 (16) | 0.0509 (14) | |
H1A | 0.3236 | 0.6460 | 0.3975 | 0.061* | |
H1B | 0.3025 | 0.6377 | 0.0715 | 0.061* | |
C2 | 0.30797 (10) | 0.56493 (19) | 0.3227 (12) | 0.0406 (13) | |
C3 | 0.28709 (10) | 0.53046 (19) | 0.1995 (15) | 0.0462 (13) | |
H3 | 0.2705 | 0.5489 | 0.1014 | 0.055* | |
C4 | 0.29008 (10) | 0.47354 (18) | 0.2199 (15) | 0.0445 (12) | |
H4 | 0.2747 | 0.4522 | 0.1438 | 0.053* | |
C5 | 0.31403 (10) | 0.45058 (19) | 0.3654 (11) | 0.0382 (13) | |
C6 | 0.33463 (9) | 0.48542 (18) | 0.4878 (16) | 0.0431 (12) | |
H5 | 0.3529 | 0.4723 | 0.5831 | 0.052* | |
C7 | 0.33114 (10) | 0.54225 (18) | 0.4641 (15) | 0.0419 (12) | |
H6 | 0.3468 | 0.5646 | 0.5513 | 0.050* | |
C8 | 0.31705 (10) | 0.38964 (19) | 0.3880 (12) | 0.0396 (13) | |
C9 | 0.29460 (11) | 0.35779 (18) | 0.5044 (18) | 0.0547 (14) | |
H9 | 0.2760 | 0.3730 | 0.5305 | 0.066* | |
C10 | 0.29691 (13) | 0.3008 (2) | 0.5284 (19) | 0.0725 (19) | |
H10 | 0.2810 | 0.2816 | 0.6064 | 0.087* | |
C11 | 0.32143 (12) | 0.2747 (2) | 0.4442 (19) | 0.0704 (18) | |
H11 | 0.3222 | 0.2371 | 0.4892 | 0.084* | |
C12 | 0.34392 (12) | 0.3043 (2) | 0.3272 (14) | 0.0566 (17) | |
H12 | 0.3607 | 0.2881 | 0.2890 | 0.068* | |
C13 | 0.34199 (10) | 0.36196 (19) | 0.2958 (14) | 0.0437 (14) | |
C14 | 0.36506 (12) | 0.3904 (2) | 0.1625 (13) | 0.0463 (15) | |
N1 | 0.38449 (10) | 0.41217 (16) | 0.0496 (14) | 0.0642 (15) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br | 0.0633 (4) | 0.0500 (3) | 0.0709 (4) | 0.0116 (3) | −0.0080 (4) | −0.0071 (4) |
C1 | 0.056 (3) | 0.042 (3) | 0.055 (4) | 0.001 (2) | −0.007 (3) | 0.005 (3) |
C2 | 0.040 (3) | 0.040 (3) | 0.042 (3) | −0.005 (2) | 0.005 (3) | 0.003 (2) |
C3 | 0.037 (3) | 0.049 (3) | 0.052 (4) | 0.006 (2) | −0.006 (3) | 0.004 (3) |
C4 | 0.039 (3) | 0.045 (3) | 0.049 (3) | −0.004 (2) | −0.006 (3) | −0.009 (3) |
C5 | 0.035 (3) | 0.041 (3) | 0.039 (3) | 0.002 (2) | 0.008 (2) | 0.000 (2) |
C6 | 0.039 (3) | 0.044 (3) | 0.046 (3) | 0.001 (2) | −0.005 (3) | −0.003 (3) |
C7 | 0.038 (3) | 0.043 (3) | 0.044 (3) | −0.003 (2) | −0.006 (3) | −0.001 (3) |
C8 | 0.035 (3) | 0.039 (3) | 0.045 (3) | −0.004 (2) | −0.001 (2) | −0.001 (2) |
C9 | 0.047 (3) | 0.046 (3) | 0.071 (4) | 0.002 (2) | 0.008 (4) | 0.002 (4) |
C10 | 0.076 (4) | 0.048 (3) | 0.094 (5) | −0.016 (3) | 0.021 (5) | 0.010 (4) |
C11 | 0.071 (4) | 0.037 (3) | 0.103 (5) | 0.000 (3) | 0.010 (5) | 0.004 (4) |
C12 | 0.064 (4) | 0.036 (3) | 0.070 (5) | 0.009 (3) | 0.000 (3) | 0.000 (3) |
C13 | 0.044 (3) | 0.037 (3) | 0.051 (4) | −0.003 (2) | −0.004 (3) | 0.001 (3) |
C14 | 0.042 (3) | 0.042 (3) | 0.055 (4) | 0.005 (2) | 0.007 (3) | −0.002 (3) |
N1 | 0.052 (3) | 0.054 (3) | 0.086 (4) | 0.001 (2) | 0.009 (3) | −0.005 (3) |
Br—C1 | 1.959 (5) | C7—H6 | 0.9830 |
C1—C2 | 1.499 (6) | C8—C9 | 1.396 (6) |
C1—H1A | 1.0754 | C8—C13 | 1.407 (6) |
C1—H1B | 0.9305 | C9—C10 | 1.389 (7) |
C2—C7 | 1.355 (6) | C9—H9 | 0.9577 |
C2—C3 | 1.388 (6) | C10—C11 | 1.364 (7) |
C3—C4 | 1.389 (6) | C10—H10 | 0.9396 |
C3—H3 | 0.9877 | C11—C12 | 1.369 (7) |
C4—C5 | 1.395 (6) | C11—H11 | 0.9303 |
C4—H4 | 0.9453 | C12—C13 | 1.407 (6) |
C5—C6 | 1.383 (6) | C12—H12 | 0.8997 |
C5—C8 | 1.486 (6) | C13—C14 | 1.401 (7) |
C6—C7 | 1.390 (6) | C14—N1 | 1.155 (6) |
C6—H5 | 1.0007 | ||
C2—C1—Br | 113.3 (4) | C2—C7—H6 | 122.6 |
C2—C1—H1A | 109.8 | C6—C7—H6 | 115.5 |
Br—C1—H1A | 106.2 | C9—C8—C13 | 117.7 (4) |
C2—C1—H1B | 113.8 | C9—C8—C5 | 119.8 (4) |
Br—C1—H1B | 99.5 | C13—C8—C5 | 122.5 (4) |
H1A—C1—H1B | 113.7 | C10—C9—C8 | 121.0 (5) |
C7—C2—C3 | 119.1 (4) | C10—C9—H9 | 116.5 |
C7—C2—C1 | 120.3 (4) | C8—C9—H9 | 121.5 |
C3—C2—C1 | 120.6 (5) | C11—C10—C9 | 120.7 (5) |
C2—C3—C4 | 120.2 (5) | C11—C10—H10 | 122.3 |
C2—C3—H3 | 116.1 | C9—C10—H10 | 117.0 |
C4—C3—H3 | 123.7 | C10—C11—C12 | 120.3 (5) |
C3—C4—C5 | 120.3 (4) | C10—C11—H11 | 116.0 |
C3—C4—H4 | 116.5 | C12—C11—H11 | 123.5 |
C5—C4—H4 | 123.1 | C11—C12—C13 | 120.2 (5) |
C6—C5—C4 | 118.9 (4) | C11—C12—H12 | 121.2 |
C6—C5—C8 | 121.1 (4) | C13—C12—H12 | 118.3 |
C4—C5—C8 | 120.1 (4) | C14—C13—C12 | 118.3 (5) |
C5—C6—C7 | 119.7 (5) | C14—C13—C8 | 121.4 (4) |
C5—C6—H5 | 123.8 | C12—C13—C8 | 120.2 (4) |
C7—C6—H5 | 116.3 | N1—C14—C13 | 177.7 (6) |
C2—C7—C6 | 121.8 (5) |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1B···Bri | 0.93 | 2.82 | 3.699 (6) | 158 |
C1—H1A···N1ii | 1.08 | 2.61 | 3.634 (8) | 159 |
C9—H9···Briii | 0.96 | 3.05 | 3.750 (6) | 131 |
Symmetry codes: (i) x, y, z−1; (ii) −x+3/4, y+1/4, z+3/4; (iii) −x+1/2, −y+1, z+1/2. |